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illrrrrrrW - Free and Open Source Software
illrrrrrrW - Free and Open Source Software
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The<br />
LOUJ-OhTn<br />
JJleter<br />
ALL RESISTORS :t~%<br />
Did you eyer try to get a good resistance<br />
read ing on a speaker voice coil?<br />
Or an automobile ignition balla st resistor? '<br />
Or a pilot light bu lb , length of coax, relay<br />
contact , loading coil, identi fy ing transformer<br />
windings, centertaps, etc .? If you<br />
have, then yo u' ve found that most ohmmet<br />
ers don' t have a rea lly low resista nc e<br />
scale - or if they do the zero set ting is<br />
unreliable and the meter scale inad equ at e.<br />
Aft er years of annoyan ce from this problem<br />
I finally decided that a low-value<br />
ohmmeter wou ld be a handy device to have<br />
around. In fact , applications for this meter<br />
just seem to suggest themselves. Why<br />
bother building a new version of an old<br />
instrument and not inc or porate new innovati<br />
ons? So I came up with the se requirements:<br />
• No zero ing knob - just a " set it<br />
and forget it" calibration cont rol.<br />
• Linear scale read ing from zero to a<br />
fixed value, rather than to inf inity.<br />
What good is infinity to an ohmmete<br />
r, besides making the upper<br />
25% or so of the scale relatively<br />
useless?<br />
• Solid terminal connectors rath er<br />
than wires with probes (optional).<br />
This would prevent poor contacts<br />
in the circui t, leading to error.<br />
The finished version uses one size D<br />
flashlight cell, has t wo scales - zero to<br />
lOQ, and zero to I Q . A " test" switch<br />
(momentary pushb utton) is used because<br />
of the high current requirem ent of the<br />
circuit. Battery life is conserved in this<br />
way.<br />
Theory of operation<br />
The circuit consists of a constant-<br />
FEBRUARY 1971<br />
A. Sch ecner W3YZ C<br />
122 She rry Lane Apts.<br />
Conshoho cken, PA 1942 8<br />
curr ent gen erator (Q 1) Lo provide a known<br />
Current through the test resistance. The<br />
voltage drop across this resistance (100 mV<br />
maximum) is read on a meter whose<br />
internal resistance is much higher than a<br />
test resistance of 10Q. Therefore , the<br />
met er does not load t he circuit.<br />
A bias for Ql is established by diodes<br />
Dl and D2 and resistors RI, R2 , R3, R4 ,<br />
and R5 . Use of the diod es hold s the bia s<br />
level constant desp ite nominal de cay of<br />
battery voltage. Diode D3 pr events severe<br />
overload of the meter in the absence of a<br />
test resistance. In case the test button is<br />
pres sed, the meter will overload, but not<br />
much, thanks to D3.<br />
My met er was "Obtained when I scrapped<br />
a Heath grid-dipper...... after bu ying a solidsta<br />
te model. The meter requiremen ts are<br />
500 IlA full scale, 200Q resista nce. A<br />
substitute may be constructed by using a<br />
mo re sensitive meter with a shun t, so long<br />
as the result is 500 IlA, 200n.<br />
Construction<br />
Layout is not critic al, but sold er connect<br />
ions must be solid and medium bus<br />
wire must be used. The battery connector<br />
mu st make tight connection with the batte<br />
ry . Check inte rn al resistance by shorting<br />
the test terminals wit h heavy wire. Pressing<br />
the test button should give a reading of<br />
zero.<br />
Transistor Q 1 may be replaced by any<br />
on e of a number of high-beta NPN typ es.<br />
Try .what yo u have around and see if it<br />
wor ks. R2 may be used to balan ce slight<br />
differences if another transistor is used.<br />
Calibrate by testing a precision IOn resi s<br />
tor (O~10Q scale) and setting the calibration<br />
control for ,a full-scale reading. The<br />
other scale should foll ow automatic ally.<br />
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